NASA Scientific and Technical Aerospace Reports
NASA Scientific and Technical Aerospace Reports
NASA Scientific and Technical Aerospace Reports
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Hydrodynamic film-riding gas seal, having been successfully used in industrial pump <strong>and</strong> compressor applications for<br />
decades, is now finding way into aero-engines. <strong>Aerospace</strong> applications require the seal work robustly under various speeds <strong>and</strong><br />
constantly changing pressures. Maintaining seal face flatness is also more challenging in aerospace than in industrial<br />
applications because of the seal size <strong>and</strong> the rapid thermal transition in aero-engines. Another difficulty in aerospace<br />
application comes from the altitude condition, where air is thin, not enough opening force may be generated to separate the<br />
seal faces from touching. Therefore, the hydrodynamic groove design is more critical in aerospace application. In order to<br />
maximize the seal performances, the groove shape <strong>and</strong> depth are optimized for the worst application condition, such as at the<br />
altitude, with using a 2D model coupled with a non-linear optimization procedure. Seals designed in this way have been found<br />
working well both in rig test <strong>and</strong> in on-flight evaluation. However, two recently designed seals based on full optimization were<br />
found not working during rig test. These two seals features very fine grooves that is thinner than the other seals that worked<br />
well. The 2D code from time to time predicted that seals work better if more grooves were engraved. The under-performed<br />
two seals indicated there might be something missing in the 2D model. It was speculated that the entrance losses <strong>and</strong> 3D effects<br />
for narrow grooves become significant, resulting in reduction of hydrodynamic opening force. In order to quantify the<br />
influences of 3D effect, a three-dimensional model is therefore developed to calculate the fluid flow between the seal faces,<br />
<strong>and</strong> then the results are compared with the 2D solution. The model solves a circumferential section of seal face that consists<br />
one l<strong>and</strong> <strong>and</strong> one groove region. A small region outside the sealing face is also included to simulate the flow entrance <strong>and</strong> exit.<br />
It was found that the 3D CFD model generally agrees with the 2D model in determining the optimum groove dimensions. The<br />
3D code gives similar trend predictions of seal opening force under the influences of groove depth, number of grooves, l<strong>and</strong><br />
to groove ratio <strong>and</strong> groove angle, although there exist differences in the absolute value levels. The 3D CFD results forced a<br />
re-examination of hardware <strong>and</strong> further re-test the seal. It is concluded that the problems were due to manufacture tolerance<br />
with such fine grooves. The design code is correct, but manufacture capability should be incorporated. CFD results <strong>and</strong> test<br />
data are reported in this paper.<br />
Author<br />
Computational Fluid Dynamics; Sealing; Two Dimensional Models; Three Dimensional Models; Fluid Flow; <strong>Aerospace</strong><br />
Engineering<br />
20060002385 Advanced Products Co., CT, USA<br />
High-Temperature Metallic Seal Development for Aero Propulsion <strong>and</strong> Gas Turbine Applications<br />
More, Greg; Datta, Amit; 2004 <strong>NASA</strong> Seal/Secondary Air System Workshop, Volume 1; October 2005, pp. 1-18; In English;<br />
See also 20060002371; Original contains color illustrations; No Copyright; Avail.: CASI: A03, Hardcopy<br />
An innovative seal consisting of a blade alloy spring energizer <strong>and</strong> cold formable superalloy jacket can be designed for<br />
applications above 1500 F. The seal is expected to minimize cooling air <strong>and</strong> leakage thereby enhancing engine efficiency. The<br />
design can be further improved with cast net shape single crystal springs attached to an easily machinable superalloy ring. The<br />
single crystal spring structure can also be used where low load/ high deflection device is required for extremely high<br />
temperature applications.<br />
Derived from text<br />
High Temperature; Seals (Stoppers); Loads (Forces); Leakage; Heat Resistant Alloys; Crystal Structure; Single Crystals<br />
20060002461 Lawrence Livermore National Lab., Livermore, CA USA<br />
Dimensional Measurements of Three Tubes by Computed Tomography<br />
Schneberk, D. J.; Martz, H. E.; Brown, W. D.; Oct. 13, 2004; 12 pp.; In English<br />
Report No.(s): DE2005-15014597; UCRL-TR-207195; No Copyright; Avail.: Department of Energy Information Bridge<br />
Low density polyethylene (LDPE), copper (Cu), <strong>and</strong> gold (Au) tubes were scanned on KCAT to identify <strong>and</strong> evaluate the<br />
impact of phase effects on quantitative object recovery. These tubes are phantoms for high energy density capsules. Digital<br />
radiographs for each tube are shown in Figure 1. The LDPE tube was scanned at 60 kV, while the Cu <strong>and</strong> the Au tubes were<br />
scanned at 140 kV. All tubes were scanned at a magnification of 3, with approximately 100-mm distance between the exit plane<br />
of the tube <strong>and</strong> the scintillator. Notice the prominence of the outer bright <strong>and</strong> inner dark edges for the LDPE tube DR, <strong>and</strong><br />
their absence from the Cu <strong>and</strong> Au tube DRs. The bright <strong>and</strong> dark edges are a result of change in phase of the x-rays. The x-ray<br />
fluence is partly attenuated <strong>and</strong> partly refracted. The location near the outer edge of the tube appears to be more attenuating<br />
since those x-rays have refracted to locations just outside the tube. Alternatively, the added counts from the refraction result<br />
in intensities that are greater than the incident intensity effectively representing a negative attenuation. This results in more<br />
counts in that location than in the incident intensity image violating the positivedefinite requirement for st<strong>and</strong>ard CT<br />
reconstruction methodologies. One aspect of our CT processing techniques remove some of this signal on the outside of the<br />
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